Surface-induced resistivity of thin metallic films bounded by a rough fractal surface
Author
dc.contributor.author
Munoz, Raúl C.
Author
dc.contributor.author
Finger, Ricardo
Author
dc.contributor.author
Arenas, Claudio
Author
dc.contributor.author
Kremer, German
Author
dc.contributor.author
Moraga, Luis
Admission date
dc.date.accessioned
2018-12-20T14:26:49Z
Available date
dc.date.available
2018-12-20T14:26:49Z
Publication date
dc.date.issued
2002
Cita de ítem
dc.identifier.citation
Physical Review B - Condensed Matter and Materials Physics, Volumen 66, Issue 20, 2018, Pages 2054011-2054019
Identifier
dc.identifier.issn
01631829
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/156017
Abstract
dc.description.abstract
We have extended the modified formalism of Sheng, Xing, and Wang [J. Phys.: Condens. Matter 11 L299 (1999)] to allow the calculation of the conductivity of a thin metallic film bounded by a rough fractal surface. We utilized the so-called k-correlation model proposed by Palasantzas and Barnas [Phys. Rev. B 48, 14472 (1993); 56, 7726 (1997)], to describe the height-height autocorrelation function corresponding to a self-affine roughness. This extension permits the calculation of the conductivity of the film as a function of the r.m.s. roughness amplitude δ, of the lateral correlation length ξ, of the mean free path in the bulk l, and of the roughness exponent H. We found that the degree of surface irregularity, represented by the roughness exponent H characterizing the surface, does influence the conductivity of the film, as first discovered by Palasantzas and Barnas. However, this influence manifests itself for large bulk mean free paths l ≈ 1000 nm and for large correlation lengths ξ≈